With these data about the strata, together with the lists of possible \(\lbrace \Delta _{u_i}\rbrace \)  identified before, we are now ready to proceed to the next step.
Let us denote the set of all Coulomb branch strata as \({\cal I}= \lbrace  {\cal I}_a\rbrace \) , and the set of strata carrying the UV simple flavor factor \(\mathfrak {g}_i\)  by \({\cal I}_{\mathfrak {g}_i} \subset {\cal I}\) . We may now make use of the following formulas relating the data of the theory at the origin to the data of the theories living on each stratum (in the absence of flavor symmetry enhancements) [1]}, [2]}:
\(h_{\mathrm {ECB}} &=& 12 c_{\mathrm {4d}}- 2r - \sum _{{\cal I}_a \in {\cal I}} b_a \,\Delta _a^{\mathrm {sing}}~,\nonumber \\k_{\mathfrak {g}_i} &=& \sum _{{\cal I}_a \in {\cal I}_{\mathfrak {g}_i}} {\Delta _a^{\mathrm {sing}} \over \Delta _a} [k_a - T^i(\mathbf {R}_a)]+ T^i(\mathbf {R})~,\,\,\,\,\,\) 
